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1 // 2 // ******************************************************************** 3 // * License and Disclaimer * 4 // * * 5 // * The Geant4 software is copyright of the Copyright Holders of * 6 // * the Geant4 Collaboration. It is provided under the terms and * 7 // * conditions of the Geant4 Software License, included in the file * 8 // * LICENSE and available at http://cern.ch/geant4/license . These * 9 // * include a list of copyright holders. * 10 // * * 11 // * Neither the authors of this software system, nor their employing * 12 // * institutes,nor the agencies providing financial support for this * 13 // * work make any representation or warranty, express or implied, * 14 // * regarding this software system or assume any liability for its * 15 // * use. Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitation of liability. * 17 // * * 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************************************** 25 // 26 // 27 // 28 // Author: Alexander Bagulya 29 // 11 March 2012 30 // on the base of G4LivermoreComptonModel 31 // 32 // History: 33 // -------- 34 // 18 Apr 2009 V Ivanchenko Cleanup initialisation and generation of secondaries: 35 // - apply internal high-energy limit only in constructor 36 // - do not apply low-energy limit (default is 0) 37 // - remove GetMeanFreePath method and table 38 // - added protection against numerical problem in energy sampling 39 // - use G4ElementSelector 40 // 26 Dec 2010 V Ivanchenko Load data tables only once to avoid memory leak 41 42 #include "G4LivermoreComptonModel.hh" 43 44 #include "G4AtomicShell.hh" 45 #include "G4AutoLock.hh" 46 #include "G4DopplerProfile.hh" 47 #include "G4Electron.hh" 48 #include "G4Exp.hh" 49 #include "G4Log.hh" 50 #include "G4LossTableManager.hh" 51 #include "G4ParticleChangeForGamma.hh" 52 #include "G4PhysicalConstants.hh" 53 #include "G4ShellData.hh" 54 #include "G4SystemOfUnits.hh" 55 #include "G4VAtomDeexcitation.hh" 56 57 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 58 59 namespace 60 { 61 G4Mutex LivermoreComptonModelMutex = G4MUTEX_INITIALIZER; 62 } 63 using namespace std; 64 65 G4PhysicsFreeVector* G4LivermoreComptonModel::data[] = {nullptr}; 66 G4ShellData* G4LivermoreComptonModel::shellData = nullptr; 67 G4DopplerProfile* G4LivermoreComptonModel::profileData = nullptr; 68 G4String G4LivermoreComptonModel::gDataDirectory = ""; 69 70 static const G4double ln10 = G4Log(10.); 71 72 G4LivermoreComptonModel::G4LivermoreComptonModel(const G4ParticleDefinition*, const G4String& nam) 73 : G4VEmModel(nam) 74 { 75 fParticleChange = nullptr; 76 verboseLevel = 1; 77 // Verbosity scale: 78 // 0 = nothing 79 // 1 = warning for energy non-conservation 80 // 2 = details of energy budget 81 // 3 = calculation of cross sections, file openings, sampling of atoms 82 // 4 = entering in methods 83 84 if (verboseLevel > 1) { 85 G4cout << "Livermore Compton model is constructed " << G4endl; 86 } 87 88 // Mark this model as "applicable" for atomic deexcitation 89 SetDeexcitationFlag(true); 90 91 fParticleChange = nullptr; 92 fAtomDeexcitation = nullptr; 93 } 94 95 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 96 97 G4LivermoreComptonModel::~G4LivermoreComptonModel() 98 { 99 if (IsMaster()) { 100 delete shellData; 101 shellData = nullptr; 102 delete profileData; 103 profileData = nullptr; 104 for (G4int i = 0; i <= maxZ; ++i) { 105 if (data[i]) { 106 delete data[i]; 107 data[i] = nullptr; 108 } 109 } 110 } 111 } 112 113 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 114 115 void G4LivermoreComptonModel::Initialise(const G4ParticleDefinition* particle, 116 const G4DataVector& cuts) 117 { 118 if (verboseLevel > 1) { 119 G4cout << "Calling G4LivermoreComptonModel::Initialise()" << G4endl; 120 } 121 122 // Initialise element selector 123 if (IsMaster()) { 124 // Initialise element selector 125 InitialiseElementSelectors(particle, cuts); 126 127 // Access to elements 128 const G4ElementTable* elemTable = G4Element::GetElementTable(); 129 size_t numElems = (*elemTable).size(); 130 for (size_t ie = 0; ie < numElems; ++ie) { 131 const G4Element* elem = (*elemTable)[ie]; 132 const G4int Z = std::min(maxZ, elem->GetZasInt()); 133 if (data[Z] == nullptr) { 134 ReadData(Z); 135 } 136 } 137 138 // For Doppler broadening 139 if (shellData == nullptr) { 140 shellData = new G4ShellData(); 141 shellData->SetOccupancyData(); 142 G4String file = "/doppler/shell-doppler"; 143 shellData->LoadData(file); 144 } 145 if (profileData == nullptr) { 146 profileData = new G4DopplerProfile(); 147 } 148 } 149 150 if (verboseLevel > 2) { 151 G4cout << "Loaded cross section files" << G4endl; 152 } 153 154 if (verboseLevel > 1) { 155 G4cout << "G4LivermoreComptonModel is initialized " << G4endl 156 << "Energy range: " << LowEnergyLimit() / eV << " eV - " << HighEnergyLimit() / GeV 157 << " GeV" << G4endl; 158 } 159 // 160 if (isInitialised) { 161 return; 162 } 163 164 fParticleChange = GetParticleChangeForGamma(); 165 fAtomDeexcitation = G4LossTableManager::Instance()->AtomDeexcitation(); 166 isInitialised = true; 167 } 168 169 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 170 171 void G4LivermoreComptonModel::InitialiseLocal(const G4ParticleDefinition*, G4VEmModel* masterModel) 172 { 173 SetElementSelectors(masterModel->GetElementSelectors()); 174 } 175 176 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 177 178 const G4String& G4LivermoreComptonModel::FindDirectoryPath() 179 { 180 // no check in this method - environment variable is check by utility 181 if (gDataDirectory.empty()) { 182 auto param = G4EmParameters::Instance(); 183 std::ostringstream ost; 184 if (param->LivermoreDataDir() == "livermore") { 185 ost << param->GetDirLEDATA() << "/livermore/comp/"; 186 } 187 else { 188 ost << param->GetDirLEDATA() << "/epics2017/comp/"; 189 } 190 gDataDirectory = ost.str(); 191 } 192 return gDataDirectory; 193 } 194 195 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 196 197 void G4LivermoreComptonModel::ReadData(const G4int ZZ) 198 { 199 if (verboseLevel > 1) { 200 G4cout << "G4LivermoreComptonModel::ReadData()" << G4endl; 201 } 202 const G4int Z = std::min(ZZ, maxZ); 203 204 if (data[Z] != nullptr) { 205 return; 206 } 207 208 data[Z] = new G4PhysicsFreeVector(); 209 210 std::ostringstream ost; 211 ost << FindDirectoryPath() << "ce-cs-" << Z << ".dat"; 212 213 std::ifstream fin(ost.str().c_str()); 214 215 if (!fin.is_open()) { 216 G4ExceptionDescription ed; 217 ed << "G4LivermoreComptonModel data file <" << ost.str().c_str() << "> is not opened!" 218 << G4endl; 219 G4Exception("G4LivermoreComptonModel::ReadData()", "em0003", FatalException, ed, 220 "G4LEDATA version should be G4EMLOW8.0 or later"); 221 return; 222 } 223 else { 224 if (verboseLevel > 3) { 225 G4cout << "File " << ost.str() << " is opened by G4LivermoreComptonModel" << G4endl; 226 } 227 data[Z]->Retrieve(fin, true); 228 data[Z]->ScaleVector(MeV, MeV * barn); 229 } 230 fin.close(); 231 } 232 233 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 234 235 G4double G4LivermoreComptonModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*, 236 G4double GammaEnergy, G4double Z, 237 G4double, G4double, G4double) 238 { 239 if (verboseLevel > 3) { 240 G4cout << "G4LivermoreComptonModel::ComputeCrossSectionPerAtom()" << G4endl; 241 } 242 G4double cs = 0.0; 243 244 if (GammaEnergy < LowEnergyLimit()) { 245 return 0.0; 246 } 247 248 G4int intZ = G4lrint(Z); 249 if (intZ < 1 || intZ > maxZ) { 250 return cs; 251 } 252 253 G4PhysicsFreeVector* pv = data[intZ]; 254 255 // if element was not initialised 256 // do initialisation safely for MT mode 257 if (pv == nullptr) { 258 InitialiseForElement(nullptr, intZ); 259 pv = data[intZ]; 260 if (pv == nullptr) { 261 return cs; 262 } 263 } 264 265 auto n = G4int(pv->GetVectorLength() - 1); 266 G4double e1 = pv->Energy(0); 267 G4double e2 = pv->Energy(n); 268 269 if (GammaEnergy <= e1) { 270 cs = GammaEnergy / (e1 * e1) * pv->Value(e1); 271 } 272 else if (GammaEnergy <= e2) { 273 cs = pv->Value(GammaEnergy) / GammaEnergy; 274 } 275 else if (GammaEnergy > e2) { 276 cs = pv->Value(e2) / GammaEnergy; 277 } 278 279 return cs; 280 } 281 282 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 283 284 void G4LivermoreComptonModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect, 285 const G4MaterialCutsCouple* couple, 286 const G4DynamicParticle* aDynamicGamma, G4double, 287 G4double) 288 { 289 // The scattered gamma energy is sampled according to Klein - Nishina 290 // formula then accepted or rejected depending on the Scattering Function 291 // multiplied by factor from Klein - Nishina formula. 292 // Expression of the angular distribution as Klein Nishina 293 // angular and energy distribution and Scattering fuctions is taken from 294 // D. E. Cullen "A simple model of photon transport" Nucl. Instr. Meth. 295 // Phys. Res. B 101 (1995). Method of sampling with form factors is different 296 // data are interpolated while in the article they are fitted. 297 // Reference to the article is from J. Stepanek New Photon, Positron 298 // and Electron Interaction Data for GEANT in Energy Range from 1 eV to 10 299 // TeV (draft). 300 // The random number techniques of Butcher & Messel are used 301 // (Nucl Phys 20(1960),15). 302 303 G4double photonEnergy0 = aDynamicGamma->GetKineticEnergy(); 304 305 if (verboseLevel > 3) { 306 G4cout << "G4LivermoreComptonModel::SampleSecondaries() E(MeV)= " << photonEnergy0 / MeV 307 << " in " << couple->GetMaterial()->GetName() << G4endl; 308 } 309 310 // do nothing below the threshold 311 // should never get here because the XS is zero below the limit 312 if (photonEnergy0 < LowEnergyLimit()) return; 313 314 G4double e0m = photonEnergy0 / electron_mass_c2; 315 G4ParticleMomentum photonDirection0 = aDynamicGamma->GetMomentumDirection(); 316 317 // Select randomly one element in the current material 318 const G4ParticleDefinition* particle = aDynamicGamma->GetDefinition(); 319 const G4Element* elm = SelectRandomAtom(couple, particle, photonEnergy0); 320 321 G4int Z = elm->GetZasInt(); 322 323 G4double epsilon0Local = 1. / (1. + 2. * e0m); 324 G4double epsilon0Sq = epsilon0Local * epsilon0Local; 325 G4double alpha1 = -G4Log(epsilon0Local); 326 G4double alpha2 = 0.5 * (1. - epsilon0Sq); 327 328 G4double wlPhoton = h_Planck * c_light / photonEnergy0; 329 330 // Sample the energy of the scattered photon 331 G4double epsilon; 332 G4double epsilonSq; 333 G4double oneCosT; 334 G4double sinT2; 335 G4double gReject; 336 337 if (verboseLevel > 3) { 338 G4cout << "Started loop to sample gamma energy" << G4endl; 339 } 340 341 do { 342 if (alpha1 / (alpha1 + alpha2) > G4UniformRand()) { 343 epsilon = G4Exp(-alpha1 * G4UniformRand()); 344 epsilonSq = epsilon * epsilon; 345 } 346 else { 347 epsilonSq = epsilon0Sq + (1. - epsilon0Sq) * G4UniformRand(); 348 epsilon = std::sqrt(epsilonSq); 349 } 350 351 oneCosT = (1. - epsilon) / (epsilon * e0m); 352 sinT2 = oneCosT * (2. - oneCosT); 353 G4double x = std::sqrt(oneCosT / 2.) * cm / wlPhoton; 354 G4double scatteringFunction = ComputeScatteringFunction(x, Z); 355 gReject = (1. - epsilon * sinT2 / (1. + epsilonSq)) * scatteringFunction; 356 357 } while (gReject < G4UniformRand() * Z); 358 359 G4double cosTheta = 1. - oneCosT; 360 G4double sinTheta = std::sqrt(sinT2); 361 G4double phi = twopi * G4UniformRand(); 362 G4double dirx = sinTheta * std::cos(phi); 363 G4double diry = sinTheta * std::sin(phi); 364 G4double dirz = cosTheta; 365 366 // Doppler broadening - Method based on: 367 // Y. Namito, S. Ban and H. Hirayama, 368 // "Implementation of the Doppler Broadening of a Compton-Scattered Photon 369 // into the EGS4 Code", NIM A 349, pp. 489-494, 1994 370 371 // Maximum number of sampling iterations 372 static G4int maxDopplerIterations = 1000; 373 G4double bindingE = 0.; 374 G4double photonEoriginal = epsilon * photonEnergy0; 375 G4double photonE = -1.; 376 G4int iteration = 0; 377 G4double eMax = photonEnergy0; 378 379 G4int shellIdx = 0; 380 381 if (verboseLevel > 3) { 382 G4cout << "Started loop to sample broading" << G4endl; 383 } 384 385 do { 386 ++iteration; 387 // Select shell based on shell occupancy 388 shellIdx = shellData->SelectRandomShell(Z); 389 bindingE = shellData->BindingEnergy(Z, shellIdx); 390 391 if (verboseLevel > 3) { 392 G4cout << "Shell ID= " << shellIdx << " Ebind(keV)= " << bindingE / keV << G4endl; 393 } 394 395 eMax = photonEnergy0 - bindingE; 396 397 // Randomly sample bound electron momentum 398 // (memento: the data set is in Atomic Units) 399 G4double pSample = profileData->RandomSelectMomentum(Z, shellIdx); 400 if (verboseLevel > 3) { 401 G4cout << "pSample= " << pSample << G4endl; 402 } 403 // Rescale from atomic units 404 G4double pDoppler = pSample * fine_structure_const; 405 G4double pDoppler2 = pDoppler * pDoppler; 406 G4double var2 = 1. + oneCosT * e0m; 407 G4double var3 = var2 * var2 - pDoppler2; 408 G4double var4 = var2 - pDoppler2 * cosTheta; 409 G4double var = var4 * var4 - var3 + pDoppler2 * var3; 410 if (var > 0.) { 411 G4double varSqrt = std::sqrt(var); 412 G4double scale = photonEnergy0 / var3; 413 // Random select either root 414 if (G4UniformRand() < 0.5) { 415 photonE = (var4 - varSqrt) * scale; 416 } 417 else { 418 photonE = (var4 + varSqrt) * scale; 419 } 420 } 421 else { 422 photonE = -1.; 423 } 424 } while (iteration <= maxDopplerIterations && photonE > eMax); 425 426 // End of recalculation of photon energy with Doppler broadening 427 // Revert to original if maximum number of iterations threshold 428 // has been reached 429 if (iteration >= maxDopplerIterations) { 430 photonE = photonEoriginal; 431 bindingE = 0.; 432 } 433 434 // Update G4VParticleChange for the scattered photon 435 G4ThreeVector photonDirection1(dirx, diry, dirz); 436 photonDirection1.rotateUz(photonDirection0); 437 fParticleChange->ProposeMomentumDirection(photonDirection1); 438 439 G4double photonEnergy1 = photonE; 440 441 if (photonEnergy1 > 0.) { 442 fParticleChange->SetProposedKineticEnergy(photonEnergy1); 443 } 444 else { 445 // photon absorbed 446 photonEnergy1 = 0.; 447 fParticleChange->SetProposedKineticEnergy(0.); 448 fParticleChange->ProposeTrackStatus(fStopAndKill); 449 fParticleChange->ProposeLocalEnergyDeposit(photonEnergy0); 450 return; 451 } 452 453 // Kinematics of the scattered electron 454 G4double eKineticEnergy = photonEnergy0 - photonEnergy1 - bindingE; 455 456 // protection against negative final energy: no e- is created 457 if (eKineticEnergy < 0.0) { 458 fParticleChange->ProposeLocalEnergyDeposit(photonEnergy0 - photonEnergy1); 459 return; 460 } 461 462 G4double eTotalEnergy = eKineticEnergy + electron_mass_c2; 463 464 G4double electronE = photonEnergy0 * (1. - epsilon) + electron_mass_c2; 465 G4double electronP2 = electronE * electronE - electron_mass_c2 * electron_mass_c2; 466 G4double sinThetaE = -1.; 467 G4double cosThetaE = 0.; 468 if (electronP2 > 0.) { 469 cosThetaE = (eTotalEnergy + photonEnergy1) * (1. - epsilon) / std::sqrt(electronP2); 470 sinThetaE = -1. * sqrt(1. - cosThetaE * cosThetaE); 471 } 472 473 G4double eDirX = sinThetaE * std::cos(phi); 474 G4double eDirY = sinThetaE * std::sin(phi); 475 G4double eDirZ = cosThetaE; 476 477 G4ThreeVector eDirection(eDirX, eDirY, eDirZ); 478 eDirection.rotateUz(photonDirection0); 479 auto dp = new G4DynamicParticle(G4Electron::Electron(), eDirection, eKineticEnergy); 480 fvect->push_back(dp); 481 482 // sample deexcitation 483 if (verboseLevel > 3) { 484 G4cout << "Started atomic de-excitation " << fAtomDeexcitation << G4endl; 485 } 486 487 if (nullptr != fAtomDeexcitation && iteration < maxDopplerIterations) { 488 G4int index = couple->GetIndex(); 489 if (fAtomDeexcitation->CheckDeexcitationActiveRegion(index)) { 490 size_t nbefore = fvect->size(); 491 auto as = G4AtomicShellEnumerator(shellIdx); 492 const G4AtomicShell* shell = fAtomDeexcitation->GetAtomicShell(Z, as); 493 fAtomDeexcitation->GenerateParticles(fvect, shell, Z, index); 494 size_t nafter = fvect->size(); 495 if (nafter > nbefore) { 496 for (size_t i = nbefore; i < nafter; ++i) { 497 // Check if there is enough residual energy 498 if (bindingE >= ((*fvect)[i])->GetKineticEnergy()) { 499 // Ok, this is a valid secondary: keep it 500 bindingE -= ((*fvect)[i])->GetKineticEnergy(); 501 } 502 else { 503 // Invalid secondary: not enough energy to create it! 504 // Keep its energy in the local deposit 505 delete (*fvect)[i]; 506 (*fvect)[i] = nullptr; 507 } 508 } 509 } 510 } 511 } 512 bindingE = std::max(bindingE, 0.0); 513 fParticleChange->ProposeLocalEnergyDeposit(bindingE); 514 } 515 516 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 517 518 G4double G4LivermoreComptonModel::ComputeScatteringFunction(G4double x, G4int Z) 519 { 520 G4double value = Z; 521 if (x <= ScatFuncFitParam[Z][3]) { 522 G4double lgq = G4Log(x) / ln10; 523 524 if (lgq < ScatFuncFitParam[Z][1]) { 525 value = ScatFuncFitParam[Z][4] + lgq * ScatFuncFitParam[Z][5]; 526 } 527 else if (lgq >= ScatFuncFitParam[Z][1] && lgq < ScatFuncFitParam[Z][2]) { 528 value = ScatFuncFitParam[Z][6] 529 + lgq 530 * (ScatFuncFitParam[Z][7] 531 + lgq 532 * (ScatFuncFitParam[Z][8] 533 + lgq * (ScatFuncFitParam[Z][9] + lgq * ScatFuncFitParam[Z][10]))); 534 } 535 else { 536 value = ScatFuncFitParam[Z][11] 537 + lgq 538 * (ScatFuncFitParam[Z][12] 539 + lgq 540 * (ScatFuncFitParam[Z][13] 541 + lgq * (ScatFuncFitParam[Z][14] + lgq * ScatFuncFitParam[Z][15]))); 542 } 543 value = G4Exp(value * ln10); 544 } 545 // G4cout << " value= " << value << G4endl; 546 return value; 547 } 548 549 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 550 551 void G4LivermoreComptonModel::InitialiseForElement(const G4ParticleDefinition*, G4int Z) 552 { 553 G4AutoLock l(&LivermoreComptonModelMutex); 554 if (data[Z] == nullptr) { 555 ReadData(Z); 556 } 557 l.unlock(); 558 } 559 560 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 561 562 // Fitting data to compute scattering function based on EPICS2017 563 const G4double G4LivermoreComptonModel::ScatFuncFitParam[101][16] = { 564 {0, 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.}, 565 {1, 6.000000000e+00, 7.087999300e+00, 1.499680000e+08, -1.435559123e+01, 2.000000043e+00, 566 -3.925518125e+02, 2.434944521e+02, -5.784393623e+01, 6.160181204e+00, -2.461326602e-01, 567 -1.649463594e+03, 8.121933215e+02, -1.498313316e+02, 1.227279742e+01, -3.765996345e-01}, 568 {2, 6.000000000e+00, 7.199000403e+00, 2.500350000e+08, -1.430103027e+01, 2.000000041e+00, 569 3.574019365e+02, -1.978574937e+02, 3.971327838e+01, -3.443224867e+00, 1.091825227e-01, 570 -4.009960832e+02, 1.575831469e+02, -2.174763446e+01, 1.185163045e+00, -1.814503741e-02}, 571 {3, 6.000000000e+00, 7.301000136e+00, 3.999450000e+08, -1.357675458e+01, 2.000000074e+00, 572 7.051635443e+02, -4.223841786e+02, 9.318729225e+01, -9.002642767e+00, 3.220625771e-01, 573 1.524679907e+03, -7.851479582e+02, 1.509941052e+02, -1.285477984e+01, 4.089348830e-01}, 574 {4, 6.000000000e+00, 7.349500202e+00, 5.000350000e+08, -1.375202671e+01, 1.999999994e+00, 575 -1.832909604e+02, 1.193997722e+02, -3.034328318e+01, 3.471545044e+00, -1.484222463e-01, 576 1.397476657e+03, -7.026416933e+02, 1.320720559e+02, -1.099824430e+01, 3.424610532e-01}, 577 {5, 6.000000000e+00, 7.388999972e+00, 5.997910000e+08, -1.380548571e+01, 2.000000004e+00, 578 -2.334197545e+02, 1.467013466e+02, -3.574851109e+01, 3.925047955e+00, -1.616186492e-01, 579 6.784713308e+02, -3.419562074e+02, 6.433945831e+01, -5.354244209e+00, 1.663784966e-01}, 580 {6, 6.000000000e+00, 7.422500001e+00, 6.998420000e+08, -1.388639003e+01, 1.999999863e+00, 581 -2.460254935e+02, 1.516613633e+02, -3.622024219e+01, 3.900099543e+00, -1.576557530e-01, 582 -1.610185428e+02, 7.010907070e+01, -1.142375397e+01, 8.303365180e-01, -2.273786010e-02}, 583 {7, 6.000000000e+00, 7.451499931e+00, 7.998340000e+08, -1.388605429e+01, 1.999999612e+00, 584 -3.054540719e+02, 1.877740247e+02, -4.440273010e+01, 4.718886370e+00, -1.881615004e-01, 585 -2.263864349e+02, 1.017885461e+02, -1.716982752e+01, 1.292954622e+00, -3.668301946e-02}, 586 {8, 6.000000000e+00, 7.451499931e+00, 7.998340000e+08, -1.395860675e+01, 1.999999906e+00, 587 -3.877174895e+02, 2.345831969e+02, -5.431822300e+01, 5.643262324e+00, -2.200840540e-01, 588 -7.949384302e+02, 3.757293602e+02, -6.661741851e+01, 5.256265086e+00, -1.556986777e-01}, 589 {9, 6.000000000e+00, 7.451499931e+00, 7.998340000e+08, -1.400000063e+01, 2.000000106e+00, 590 -2.939854827e+02, 1.784214589e+02, -4.168473845e+01, 4.377669850e+00, -1.724300716e-01, 591 -1.169326170e+03, 5.545642014e+02, -9.863024948e+01, 7.801721240e+00, -2.315522357e-01}, 592 {10, 6.000000000e+00, 7.451499931e+00, 7.998340000e+08, -1.404575854e+01, 2.000000178e+00, 593 -2.615701853e+02, 1.582596311e+02, -3.698114811e+01, 3.889093901e+00, -1.533613504e-01, 594 -1.275287356e+03, 6.022076554e+02, -1.066410301e+02, 8.398773148e+00, -2.481899800e-01}, 595 {11, 6.000000000e+00, 7.500000000e+00, 1.000000000e+09, -1.344369665e+01, 1.999999860e+00, 596 1.112662501e+03, -6.807056448e+02, 1.545837472e+02, -1.548462180e+01, 5.785425068e-01, 597 -1.007702307e+03, 4.699937040e+02, -8.220352105e+01, 6.396099420e+00, -1.867816054e-01}, 598 {12, 6.000000000e+00, 7.500000000e+00, 1.000000000e+09, -1.339794047e+01, 2.000000080e+00, 599 9.895649717e+02, -5.983228286e+02, 1.340681576e+02, -1.323046651e+01, 4.863434994e-01, 600 -5.790532602e+02, 2.626052403e+02, -4.463548055e+01, 3.376239891e+00, -9.588786915e-02}, 601 {13, 6.000000000e+00, 7.587999300e+00, 1.499680000e+09, -1.340893585e+01, 2.000000078e+00, 602 7.335256091e+02, -4.405291562e+02, 9.770954287e+01, -9.519317788e+00, 3.448067237e-01, 603 -5.328832253e+02, 2.398514938e+02, -4.044557740e+01, 3.034597500e+00, -8.547410419e-02}, 604 {14, 6.000000000e+00, 7.587999300e+00, 1.499680000e+09, -1.345593195e+01, 2.000000000e+00, 605 3.978691889e+02, -2.370975001e+02, 5.158692183e+01, -4.884868277e+00, 1.707270518e-01, 606 -2.340256277e+02, 9.813362251e+01, -1.527892110e+01, 1.051070768e+00, -2.692716945e-02}, 607 {15, 6.000000000e+00, 7.587999300e+00, 1.499680000e+09, -1.349485049e+01, 2.000000083e+00, 608 2.569833671e+02, -1.513623448e+02, 3.210087153e+01, -2.925756803e+00, 9.724379436e-02, 609 -1.345727293e+01, -6.291081167e+00, 3.235960888e+00, -4.059236666e-01, 1.601245178e-02}, 610 {16, 6.000000000e+00, 7.587999300e+00, 1.499680000e+09, 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